Download Quantum Computing Lecture 1 Bits and Qubits What is Quantum

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What is Quantum Computing?
Quantum Computing
Lecture 1
Aim to use quantum mechanical phenomena that have no classical
counterpart for computational purposes.
Anuj Dawar
Central research tasks include:
• Building devices — with a specified behaviour.
• Designing algorithms — to use the behaviour.
Bits and Qubits
Mediating these two are models of computation.
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Bird’s eye view
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Why look at Quantum Computing?
• The world is quantum
A computer scientist looks at Quantum Computing:
– classical models of computation provide a level of
abstraction
Algorithmic Languages
Theory/complexity
– discrete state systems
• Devices are getting smaller
– Moore’s law
System Architecture
Specified Behaviour
Physics
– the only descriptions that work on the very small scale are
quantum
• Exploit quantum phenomena
Dragons
– using quantum phenomena may allow us to perform
computational tasks that are not otherwise possible/efficient
– understand capabilities/resources
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Course Outline
Useful Information
A total of eight lecturers.
Some useful books:
1. Bits and Qubits (this lecture).
• Nielsen, M.A. and Chuang, I.L. (2000). Quantum Computation
and Quantum Information. Cambridge University Press.
2. Linear Algebra
3. Quantum Mechanics
• Mermin, N.D. (2007). Quantum Computer Science. CUP.
4. Models of Computation
• Kitaev, A.Y., Shen, A.H. and Vyalyi, M.N. (2002). Classical
and Quantum Computation. AMS.
5. Some Applications
• Hirvensalo, M. (2004). Quantum Computing. Springer.
6. Search Algorithms
Course website:
http://www.cl.cam.ac.uk/teaching/0910/QuantComp/
7. Factorisation
8. Complexity
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Bits
Qubits
A building block of classical computational devices is a two-state
system.
0
←→
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1
Indeed, any system with a finite set of discrete, stable states, with
controlled transitions between them will do.
Quantum mechanics tells us that any such system can exist in a
superposition of states.
In general, the state of a quantum bit (or qubit for short) is
described by:
α|0i + β|1i
where, α and β are complex numbers, satisfying
|α|2 + |β|2 = 1
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Qubits
Measurement
Any attempt to measure the state
|1i
β
α|0i + β|1i
α
|0i
A qubit may be visualised as a unit vector
on the plane.
α|0i + β|1i
results in |0i with probability |α|2 , and |1i with probability |β|2 .
In general, however,
α and β are complex
numbers.
After the measurement, the system is in the measured state!
That is, further measurements will always yield the same value.
We can only extract one bit of information from the state of a
qubit.
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Measurement
α|0i + β|1i and α|0i − β|1i have
the same probabilities for their
measurement
However, they are distinct states
which behave differently in terms
of how they evolve.
Vectors
β
|1i
α|0i + β|1i
α
|0i
α|0i − β|1i
Formally, the state of a qubit is a unit vector in C2 —the
2-dimensional complex vector space.


α
 can be written as
The vector 
β
α|0i + β|1i
 
1
0
where, |0i =   and |1i =  .
0
1


|φi— a ket, Dirac notation for vectors.
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Basis
Example
Any pair of vectors |φi, |ψi ∈ C2 that are linearly independent
could serve as a basis.
The vector
"
√1
2
√1
2
#
measured in the computational basis gives
either outcome with probability 1/2.
α|0i + β|1i = α′ |φi + β ′ |ψi
Measured in the basis

The basis is determined by the measurement process or device.

Most of the time, we assume a standard (orthonormal) basis |0i
and |1i is given.
√1
2
√1
2
 
,
√1
2
−1
√
2


it gives the first outcome with probability 1.
This will be called the computational basis
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Entanglement
An n-qubit system can exist in any superposition of the 2n basis
states.
α0 |000000i + α1 |000001i + · · · + α2n −1 |111111i
P2n −1
with i=0 |αi |2 = 1
Sometimes such a state can be decomposed into the states of
individual bits
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1
1
(|00i + |01i + |10i + |11i) = √ (|0i + |1i) ⊗ √ (|0i + |1i)
2
2
2
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Entanglement
Compare the two (2-qubit) states:
1
√ (|00i + |01i) and
2
1
√ (|00i + |11i)
2
If we measure the first qubit in the first case, we see |0i with
probability 1 and the state remains unchanged.
In the second case (an EPR pair), measuring the first bit gives |0i
or |1i with equal probability. After this, the second qubit is also
determined.
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Linear Algebra
Quantum Computing
Lecture 2
The state space of a quantum system is described in terms of a
vector space.
Anuj Dawar
Vector spaces are the object of study in Linear Algebra.
In this lecture we review definitions from linear algebra that we
need in the rest of the course.
Review of Linear Algebra
We are mainly interested in vector spaces over the complex number
field – C.
We use the Dirac notation—|vi, |φi (read as ket) for vectors.
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Vector Spaces
A vector space over C is a set V with
• a commutative, associative addition operation + that has
– an identity 0: |vi + 0 = |vi
– inverses: |vi + (−|vi) = 0
• an operation of multiplication by a scalar α ∈ C such that:
– α(β|vi) = (αβ)|vi
– (α + β)|vi = α|vi + β|vi and α(|ui + |vi) = α|ui + α|vi
– 1|vi = |vi.
Cn


α1

.. 

Cn is the vector space of n-tuples of complex numbers: 
 . .
αn



α1
 .  
.  
with addition 
 . +
αn



β1
α1 + β1


.. 
..
 

. =
.

βn
αn + βn




zα1
α1
 .   . 
.   . 
and scalar multiplication z 
 . = . 
αn
zαn
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Basis
Bases for Cn

A basis of a vector space V is a minimal collection of vectors
|v1 i, . . . , |vn i such that every vector |vi ∈ V can be expressed as a
linear combination of these:
|vi = α1 |v1 i + · · · + αn |vn i.
1



The standard basis for Cn is 


0
..
.
"
3
0
(written |0i, . . . , |n − 1i).
But other bases are possible:
n—the size of the basis—is uniquely determined by V and is called
the dimension of V.
2
 
0
 
 
 
,
 
 
1
..
.
# "
4
,
0








,...,




−i
#
0
0
..
.
1







is a basis for C2 .
We’ll be interested in orthonormal bases. That is bases of vectors
of unit length that are mutually orthogonal. Examples are |0i, |1i
and √12 (|0i + |1i), √12 (|0i − |1i).
Given a basis, every vector |vi can be represented as an n-tuple of
scalars.
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Linear Operators
A linear operator A from one vector space V to another W is a
function such that:
A(α|ui + β|vi) = α(A|ui) + β(A|vi)
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Matrices
Given a choice of bases |v1 i, . . . , |vn i and |w1 i, . . . , |wm i, let
A|vj i =
m
X
αij |wi i
i=1
Then, the matrix representation of A is given by the entries αij .
If V is of dimension n and W is of dimension m, then the operator
A can be represented as an m × n-matrix.
The matrix representation depends on the choice of bases for V
and W.
Multiplying this matrix by the representation of a vector |vi in the
basis |v1 i, . . . , |vn i gives the representation of A|vi in the basis
|w1 i, . . . , |wm i.
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Examples
Inner Products
A 45◦ rotation of the real plane that takes
"
0
1
#
matrix
to
"
#
− √12
1
√
2
The operator 
0
i
of the real plane.
1
0
#
to
"
1
√
2
1
√
2
#
An inner product on V is an operation that associates to each pair
|ui, |vi of vectors a complex number
and
hu|vi.
is represented, in the standard basis by the
The operation satisfies


"
−i
0


√1
2
√1
2
− √12
√1
2

• hu|αv + βwi = αhu|vi + βhu|wi

• hu|vi = hv|ui∗ where the
∗
denotes the complex conjugate.
• hv|vi ≥ 0 (note: hv|vi is a real number) and hv|vi = 0 iff
|vi = 0.
 does not correspond to a transformation
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Inner Product on Cn
The standard inner product on Cn is obtained by taking, for
X
X
|ui =
ui |ii and |vi =
vi |ii
i
i
hu|vi =
X
u∗i vi
i
Note: hu| is a bra, which together with |vi forms the bra-ket hu|vi.
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Norms
The norm of a vector |vi (written || |vi||) is the non-negative, real
number:
p
|| |vi|| = hv|vi.
A unit vector is a vector with norm 1.
Two vectors |ui and |vi are orthogonal if hu|vi = 0.
An orthonormal basis for an inner product space V is a basis made
up of pairwise orthogonal, unit vectors.
the term Hilbert space is also used for an inner product space
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Outer Product
Eigenvalues
With a pair of vectors |ui ∈ U, |vi ∈ V we associate a linear
operator |uihv| : V → U, known as the outer product of |ui and |vi.
An eigenvector of a linear operator A : V → V is a non-zero vector
|vi such that
A|vi = λ|vi
(|uihv|)|v ′ i = hv|v ′ i|ui
for some complex number λ
λ is the eigenvalue corresponding to the eigenvector v.
|vihv| is the projection on the one-dimensional space generated by
|vi.
The eigenvalues of A are obtained as solutions of the characteristic
equation:
Any linear operator can be expressed as a linear combination of
outer products:
A=
X
det(A − λI) = 0
Each operator has at least one eigenvalue.
Aij |iihj|.
ij
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Diagonal Representation
A linear operator A is diagonalisable if
X
A=
λi |vi ihvi |
Adjoints
Associated with any linear operator A is its adjoint A† which
satisfies
hv|Awi = hA† v|wi
i
where the |vi i are an orthonormal set of eigenvectors of A with
corresponding eigenvalues λi .
In terms of matrices, A† = (A∗ )T
where ∗ denotes complex conjugation and T denotes transposition.
Equivalently, A can be written as a matrix


λ1




..


.


λn
in the basis |v1 i, . . . , |vn i of its eigenvectors.


1+i 1−i
−1
1
†

 =
1 − i −1
1+i
1


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Normal and Hermitian Operators
Unitary Operators
An operator A is said to be normal if
A linear operator A is unitary if
AA† = A† A
AA† = A† A = I
Fact: An operator is diagonalisable if, and only if, it is normal.
Unitary operators are normal and therefore diagonalisable.
A is said to be Hermitian if A = A†
Unitary operators are norm-preserving and invertible.
A normal operator is Hermitian if, and only if, it has real
eigenvalues.
hAu|Avi = hu|vi
All eigenvalues of a unitary operator have modulus 1.
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Tensor Products
If U is a vector space of dimension m and V one of dimension n
then U ⊗ V is a space of dimension mn.
Writing |uvi for the vectors in U ⊗ V:
• |(u + u′ )vi = |uvi + |u′ vi
• |u(v + v ′ )i = |uvi + |uv ′ i
• z|uvi = |(zu)vi = |u(zv)i
Given linear operators A : U → U and B : V → V, we can define
an operator A ⊗ B on U ⊗ V by
(A ⊗ B)|uvi = |(Au), (Bv)i
Tensor Products
In matrix terms,

A11 B
A12 B
···


 A21 B
A⊗B =
..


.

Am1 B
A22 B
..
.
···
..
.
Am2 B
A1m B



A2m B 




· · · Amm B
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What is Quantum Mechanics
Quantum Computing
Lecture 3
Quantum Mechanics is a framework for the development of physical
theories.
Anuj Dawar
It is not itself a physical theory.
It states four mathematical postulates that a physical theory must
satisfy.
Principles of Quantum Mechanics
Actual physical theories, such as Quantum Electrodynamics are
built upon a foundation of quantum mechanics.
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What are the Postulates About
First Postulate
The four postulates specify a general framework for describing the
behaviour of a physical system.
Associated to any physical system is a complex inner product space
(or Hilbert space) known as the state space of the system.
1. How to describe the state of a closed system.—Statics or state
space
2. How to describe the evolution of a closed system.—Dynamics
3. How to describe the interactions of a system with external
systems.—Measurement
4. How to describe the state of a composite system in terms of its
component parts.
The system is completely described at any given point in time by
its state vector, which is a unit vector in its state space.
Note: Quantum Mechanics does not prescribe what the state
space is for any given physical system. That is specified by
individual physical theories.
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Example: A Qubit
Second Postulate
Any system whose state space can be described by C2 —the
two-dimensional complex vector space—can serve as an
implementation of a qubit.
The time evolution of closed quantum system is described by the
Schrödinger equation:
Example: An electron spin.
i~
Some systems may require an infinite-dimensional state space.
d|ψi
= H|ψi
dt
where
We always assume, for the purposes of this course, that our systems
have a finite dimensional state space.
• ~ is Planck’s constant; and
• H is a fixed Hermitian operator known as the Hamiltonian of
the system.
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Second Postulate—Simpler Form
The state |ψi of a closed quantum system at time t1 is related to
the state |ψ ′ i at time t2 by a unitary operator U that depends only
on t1 and t2 .
Why Unitary?
Unitary operations are the only linear maps that preserve norm.
|ψ ′ i = U |ψi
|ψ ′ i = U |ψi
U is obtained from the Hamiltonian H by the equation:
U (t1 , t2 ) = exp[
implies
|| |ψ ′ i|| = || U |ψi|| = || |ψi|| = 1
−iH(t2 − t1 )
]
~
Exercise: Verify that unitary operations are norm-preserving.
This allows us to consider time as discrete and speak of
computational steps
Exercise: Check that if H is Hermitian, U is unitary.
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Gates, Operators, Matrices
Pauli Gates
A particularly useful set of 1-qubit gates are the Pauli Gates.
In this course, most linear operators we will be interested in are
unitary.
The X gate
They can be represented as matrices where each column is a unit
vector and columns are pairwise orthogonal.
X

X|0i = |1i X|1i = |0i
Another useful representation of unitary operators we will use is as
gates:
X=
0 1

1 0


−i
The Y gate
G
Y
A 2-qubit gate is a unitary operator on C4 .
Y |0i = i|1i Y |1i = −i|0i
Y =
0
i
0


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Pauli Gates–contd.
Third Postulate
A measurement on a quantum system has some set M of outcomes.
The Z gate
Z
Z|0i = |0i Z|1i = −|1i

Z=
1
0

0 −1



Sometimes we include the identity I = 
gate.
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1 0
0 1
 as a fourth Pauli
Quantum measurements are described by a collection
{Pm : m ∈ M } of measurement operators. These are linear (not
unitary) operators acting on the state space of the system.
If the state of the system is |ψi before the measurement, then the
probability of outcome m is:
†
p(m) = hψ|Pm
Pm |ψi
The state of the system after measurement is
q
Pm |ψi
†
hψ|Pm
Pm |ψi
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Third Postulate—contd.
Measurement in the Computational Basis
We are generally interested in the special case where the
measurement operators are projections onto a particular
orthonormal basis of the state space (which we call the
computational basis).
The measurement operators satisfy the completeness equation.
X
†
Pm
Pm = I
m∈M
So, for a single qubit, we take measurement operators P0 = |0ih0|
and P1 = |1ih1|
This guarantees that the sum of the probabilities of all outcomes
adds up to 1.
X
X
†
p(m) =
hψ|Pm
Pm |ψi = hψ|I|ψi = 1
m
This gives, for a qubit in state α|0i + β|1i:
m
p(0) = |α|2
p(1) = |β|2
Exercise: Verify!
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Global Phase
Relative Phase
√1 (|0i
2
For any state |ψi, and any θ, we can form the vector eiθ |ψi.
In contrast, consider the two states |ψ1 i =
Then, for any unitary operator U ,
Measured in the computational basis, they yield the same outcome
probabilities.
U eiθ |ψi = eiθ U |ψi
Moreover, for any measurement operator Pm
−iθ
hψ|e
†
Pm
Pm eiθ |ψi
=
†
hψ|Pm
Pm |ψi
Thus, such a global phase is unobservable and the states are
physically indistinguishable.
|ψ2 i =
√1 (|0i
2
− |1i).
+ |1i) and
However, measured in a different orthonormal basis (say
√1 (|0i + |1i) and √1 (|0i − |1i), the results are different.
2
2
Also, if H =
√1
2

1
1

1
−1

, then
H|ψ1 i = |0i H|ψ2 i = |1i
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Fourth Postulate
Separable States
The state space of a composite physical system is the tensor
product of the state spaces of the individual component physical
systems.
A state of a combined system is separable if it can be expressed as
the tensor product of states of the components.
E.g.
1
1
1
(|00i + |01i + |10i + |11i) = √ (|0i + |1i) ⊗ √ (|0i + |1i)
2
2
2
If one component is in state |ψ1 i and a second component is in
state |ψ2 i, the state of the combined system is
|ψ1 i ⊗ |ψ2 i
If Alice has a system in state |ψ1 i and Bob has a system in
state |ψ1 i, the state of their combined system is |ψ1 i ⊗ |ψ1 i.
If Alice applies U to her state, this is equivalent to
applying the operator U ⊗ I to the combined state.
Not all states of a combined system can be separated into the
tensor product of states of the individual components.
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Entangled States
The following states of a 2-qubit system cannot be separated into
components parts.
1
√ (|10i + |01i) and
2
1
√ (|00i + |11i)
2
Note: Physical separation does not imply separability. Two
particles that are physically separated could still be entangled.
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Summary
Postulate 1: A closed system is described by a unit vector in a
complex inner product space.
Postulate 2: The evolution of a closed system in a fixed time
interval is described by a unitary transform.
Postulate 3: If we measure the state |ψi of a system in an
orthonormal basis |0i · · · |n − 1i, we get the result |ji with
probability |hj|ψi|2 . After the measurement, the state of the
system is the result of the measurement.
Postulate 4: The state space of a composite system is the tensor
product of the state spaces of the components.
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Quantum Circuits
Quantum Computing
Lecture 4
A quantum circuit is a sequence of unitary operations and
measurements on an n-qubit state.





Input State
U1
U2
U3




M
Anuj Dawar
Models of Quantum Computation
Note: each Ui is described by a 2n × 2n matrix.
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Algorithms
A quantum algorithm specifies, for each n, a sequence
On = O1 . . . Ok
of n-qubit operations.
The map n → On must be computable.
i.e. the individual circuits must be generated from a
common pattern.
All measurements can be deferred to the end (possibly, at the
expense of increasing the number of qubits).
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Model of Computation
As a model of computation, this is parasitic on classical models.
what is computable is not independently determined
Purely quantum models can be defined. We will see more on this in
Lecture 8.
What computations can be performed in the model as defined?
What functions can be computed?
What decision problems are decidable?
Can all such computations be performed with some fixed set of
unitary operations?
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Simulating Boolean Gates
Computing a Function
If f : {0, 1}n → {0, 1}m is a Boolean function, the map
Could we find a quantum circuit to simulate a classical And gate?
And
b
|xi 7→ |f (x)i
a∧b
a
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may not be unitary.
We will, instead seek to implement
This would require And : |00i 7→ |0xi, |01i 7→ |0yi
|10i 7→ |0zi,
|xi ⊗ |0i 7→ |xi ⊗ |f (x)i
|11i 7→ |1wi
There is no unitary operation of this form.
Unitary operations are reversible. No information can be lost in the
process.
Exercise: Describe a unitary operation that implements the
Boolean And in this sense.
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One-Qubit Gates
We have already seen the Pauli Gates:
"
#
"
#
X=
0
1
1
0
,Y =
0
−i
i
0
,Z =
Gates on a Multi-Qubit State
"
1
0
0
−1
Another useful one-qubit gate is the Hadamard gate:


1
1
1

H=√ 
2 1 −1
H
8
#
When we draw a circuit with a one-qubit gate, this must be read as
a unitary operation on the entire state.
U
U ⊗I
This does not change measurement outcomes on the second qubit.
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Controlled Not
Controlled U
The Controlled Not is a 2-qubit gate:
|ai
|ai
|bi
|a ⊕ bi
More generally, we can define, for any single qubit operation U , the
Controlled U gate:
The controlled not flips the second qubit if the first qubit is |1i
and leaves it unchanged if it’s |0i
U
|0xi 7→ |0xi
|1xi 7→ |1, U xi
Particularly useful is the controlled-Z gate:

1 0

 0 1

C=
 0 0

0 0
0 0

Z

0 0 


0 1 

Z
1 0
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Toffoli Gate
|a1 i
|a2 i
|bi
|a1 i
The Toffoli Gate is a 3-qubit
gate.
|a2 i
It has a classical counterpart
which can be used to simulate
|(a1 · a2 ) ⊕ bi standard Boolean operations
A permutation matrix is a unitary matrix where all entries are
0 or 1.
Any 2n × 2n permutation matrix can be implemented using only
Toffoli gates.
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Classical Reversible Computation
A Boolean function f : {0, 1}n → {0, 1}n is reversible if it’s
described by a 2n × 2n permutation matrix.
For any function g : {0, 1}n → {0, 1}m , there is a reversible function
g ′ : {0, 1}m+n → {0, 1}m+n with
g ′ (x, 0) = (x, g(x)).
Toffoli gates are universal for reversible computation.
The Toffoli gate cannot be implemented using 2-bit reversible
classical gates.
13
14
Quantum Toffoli Gate
Universal Set of Gates
The Toffoli gate can be implemented using 2-qubit quantum gates.
Fact: Any unitary operation on n qubits can be implemented by a
sequence of 2-qubit operations.
Q
Q†
Q†
H
where, P =
"
Q†
Q
1
0
0
i
#
,Q =
"
1
0
0
eiπ/4
#
Q
Q†
Fact: Any unitary operation can be implemented by a combination
of C-NOTs and single qubit operations.
P
Fact: Any unitary operation can be approximated to any required
degree of accuracy using only C-NOTs, H, P and Q.
H
These can serve as our finite set of gates for quantum computation.
.
15
Deutsch-Jozsa Problem
Given a function f : {0, 1} → {0, 1}, determine whether f is
constant or balanced.
16
replacemen
Deutsch-Jozsa Algorithm
|0i
√1 (|0i
2
H
Uf
H
− |1i)
Classically, this requires two calls to the function f .
Uf with input |xi and |0i − |1i is just a phase shift.
But, if we are given the quantum black box:
|ai
|bi
One use of the box suffices
Uf
|ai
|b ⊕ f (a)i
It changes phase by (−1)f (x) .
When |xi = H|0i, this gives (−1)f (0) |0i + (−1)f (1) |1i.
Final result is [(−1)f (0) + (−1)f (1) ]|0i + [(−1)f (0) − (−1)f (1) ]|1i
which is |0i if f is constant and |1i if f is balanced.
1
2
Some Applications
Quantum Computing
Lecture 5
We look at some applications of the encoding of information in
quantum states.
Anuj Dawar
• Quantum Cryptography, or more accurately Quantum Key
Distribution.
• Superdense Coding.
Applications of Quantum Information
• Quantum Teleportation
These do not rely on quantum computation as such, but the
properties of information encoded in quantum states: superposition
and entanglement.
3
4
Quantum Key Distribution
A protocol for quantum key distribution was described by Bennett
and Brassard in 1984 (and is known as BB84).
Eve
qubit channel
Alice
Bob
classical channel
The protocol does not provide the means of transmitting an arbitrary message.
At the end of the protocol, there is a random sequence of bits that
is shared between Alice and Bob but unknown to any third party.
Assumptions
The BB84 protocol relies on the following assumptions:
• Alice has a source of random (classical) bits.
• Alice can produce qubits in states |0i and |1i.
• Alice can apply a Hadamard operator H to the qubits.
• Bob can measure incoming qubits
– either in the basis |0i, |1i;
– or in the basis
√1 (|0i
2
+ |1i),
√1 (|0i
2
− |1i).
These conditions are satisfied, for instance, by a system based on
polarised photons.
5
The Protocol
6
The Protocol–contd.
Alice sends Bob a stream of qubits.
• For each qubit, Bob randomly chooses either the basis |0i, |1i
or the basis H|0i, H|1i and measures the qubit in the chosen
basis.
For each qubit, before sending it, she
• Bob announces (over the classical channel) which basis he used
for each measurement.
• randomly chooses a bit |0i or |1i;
• randomly either applies H to the qubit or not; and
• Alice tells Bob which measurements were made in the correct
basis.
• sends it to Bob.
• The qubits which were measured in the wrong basis are
discarded, while the rest form a shared key.
So, Bob receives a random sequence of qubits, each of which is in
one of the four states:
|0i, |1i, H|0i, H|1i
7
Attacks
Why not announce the bases for all qubits before transmission,
thus avoiding the loss of half the bits?
This allows Eve to intercept, measure and re-transmit the
bits.
Why not wait until Bob has received all the qubits, then have Alice
announce the basis for each one before Bob measures them?
• Requires Bob to store the qubits—currently technically
difficult.
• If Bob can store the qubits, then Eve can too and then she can
retransmit after measurement.
If we could fix the basis before hand, this could be used to transmit
a fixed (rather than random) message.
8
Attack 2
What happens if Eve intercepts the qubits, measures each one
randomly in either the basis |0i, |1i or the basis H|0i, H|1i and
then retransmits it?
For half of the bits that are shared between Alice and Bob, Eve will
have measured them in the wrong basis.
Moreover, these bits will have changed state, and so for approx. 14
of the shared bits, the value measured by Bob will be different to
the one encoded by Alice.
Alice and Bob can choose a random sample of their shared bits and
publically check their values against each other and detect the
presence of an eavesdropper.
9
10
Attack 3
Key Distribution
Could Eve intercept the qubits, make a copy without measuring
them and re-transmit to Bob and then wait for the basis to be
announced?
Quantum key distribution relies on nothing more than
• linear superposition of states; and
• change of basis.
No Cloning Theorem:
There is no unitary operation U which for an arbitrary
state ψ gives
In particular, it does not rely on entanglement.
We next look at some applications of entanglement.
U |ψ0i = |ψψi.
Exercise: Prove the no-cloning theorem.
11
Bell States
Entanglement based protocols generally rely on using the following
four states of a two-qubit system, known as the Bell states.
1
√ (|00i + |11i),
2
1
√ (|01i + |10i)
2
1
√ (|00i − |11i),
2
1
√ (|01i − |10i)
2
These form an orthonormal basis for C4 , known as the Bell basis.
Note that, in each of the states, measuring either qubit in the
computational basis yields |0i or |1i with equal probability, but
after the measurement, the other bit is determined.
12
Generating Bell States
We can generate the Bell states from the computational basis
|00i, |01i, |10i, |11i using the following circuit:
H
√1 (|00i
2
|00i
√1 (|00i
2
+ |10i)
+ |11i)
13
Superdense Coding
14
Superdense Coding 2
In general, it is impossible to extract more than one classical bit of
information from a single qubit.
Generating Bell states from
the first qubit.
√1 (|00i + |11i)
2
with only operations on
1
1
(X ⊗ I) √ (|00i + |11i) = √ (|01i + |10i)
2
2
However, if Alice and Bob is each in possession of one qubit of a
pair in a known Bell state
1
√ (|00i + |11i)
2
1
1
(Z ⊗ I) √ (|00i + |11i) = √ (|00i − |11i)
2
2
Then Alice can perform an operation solely on her own qubit, and
then send it to Bob to convey two bits of information.
1
1
((XZ) ⊗ I) √ (|00i + |11i) = √ (|01i − |10i)
2
2
15
Superdense Coding 3
Once he has both qubits, Bob can convert back to the
computational basis using the circuit.
16
Quantum Teleportation
The superdense coding protocol allows Alice to send Bob two
classical bits by transmitting a single qubit, provided they already
share an entangled pair.
H
Conversely, the quantum teleportation protocol allows Alice to send
Bob a qubit, by sending just two classical bits along a classical
channel, provided they already share an entangled pair.
After this, a measurement in the computational basis yields the
two bits that Alice intended to convey.
Contrast this with the no-cloning theorem, which tells us that we
cannot make a copy of a qubit.
17
Quantum Teleportation 2
Alice has a state |φi that she wishes to transmit to Bob. The two
already share a pair of qubits in state √12 (|00i + |11i).
18
Quantum Teleportation 3
Alice conveys to Bob the result of her measurement. Say the qubit
in Bob’s possession is in state |θi, then:
• If Alice measures |00i, then |φi = |θi.
|φi
Entangled Pair



• If Alice measures |01i, then |φi = X|θi.
H
M
• If Alice measures |10i, then |φi = Z|θi.
• If Alice measures |11i, then |φi = XZ|θi.
Thus, Bob performs the appropriate operation and now has a qubit
whose state is exactly |φi.
1
2
Search Problems
Quantum Computing
One of the two most important algorithms in quantum computing
is Grover’s search algorithm—first presented by Lov Grover in 1996.
Lecture 6
This provides a means of searching for a particular value in an
unstructured search space.
Anuj Dawar
Compare
Quantum Searching
• searching for a name in a telephone directory
• searching for a phone number in a telephone directory
Given a black box which can take any of N inputs, and for each of
them gives a yes/no answer, Grover’s algorithm allows us to find
√
the unique value for which the answer is yes in O( N ) steps (with
high probability).
3
replacemen
4
Deutsch-Jozsa Algorithm revisited
|0i
√1 (|0i
2
H
Uf
H
− |1i)
When the lower input to Uf is |0i − |1i, we can regard this as
unchanged, and instead see Uf as shifting the phase of the upper
qubit by (−1)f (x) .
Oracle
Suppose we have f : N → {0, 1}, and that N = 2n , so we can think
of f as operating on n bits.
We assume that we are provided a black box or oracle Uf for
computing f , in the following sense:
|xi



|bi
Uf
|b ⊕ f (x)i
5
6
replacements
Grover’s Algorithm
Grover’s Algorithm Schematic
√
O( N )
Suppose further that there is exactly one n-bit value a such that
f (a) = 1
and for all other values x,
f (x) = 0.
|0i
H
|0i
H
|0i
H
|0i
H
z
}|
Uf
{
···
W
Uf
W
M
|0i−|1i
Grover’s algorithm gives us a way of using the black box Uf to
√
determine the value a with O( N ) = O(2n/2 ) calls to Uf .
The operator G = (W ⊗ I)Uf is known as the Grover Iterate (we
will see soon what W is).
The input to the last bit is
√1 (|0i
2
− |1i).
7
The Action of Uf
As the “output qubit” is |0i − |1i, it remains unaffected by the
action of Uf , which we can think of instead as a conditional phase
change on the n input qubits.
|ai 7→ −|ai
|xi 7→ |xi
for any x 6= a
We will ignore the output bit completely and instead talk of the
n-bit operator V above.
Note: V = I − 2|aiha|.
We now analyse the Grover iterate W V .
8
Components of W
We write H ⊗n for the following operation:

H






H
n inputs


H




H
And X ⊗n for the following
operation:

X






X
n inputs


X




X
Each of these can, of course, be implemented by a series of n
1-qubit operations.
9
10
More Components of W
Defining W
Now, we can define W by:
We write cZ ⊗n for the n-bit controlled-Z gate:
n inputs














cZ ⊗n
Z



=



1 0
···
0
0 1
.. ..
. .
···
..
.
0
..
.
0 0
· · · −1
W

= (−1)H ⊗n (X ⊗n cZ ⊗n X ⊗n )H ⊗n .
= (−1)H ⊗n (I − 2|0n ih0n |)H ⊗n







Write |Ψi for the state
H
cZ ⊗n can be implemented using O(n) cZ and Toffoli gates, using
some workspace qubits (Exercise).
⊗n
N −1
1 X
|0 i = √
|ii.
N i=0
n
So, W = (−1)(I − 2|ΨihΨ|), i.e.
W = 2|ΨihΨ| − I.
11
12
The Grover Iterate
Geometric View
Since G = W V , we have
We can picture the action of W and V in the two-dimensional real
plane spanned by the vectors |ai and |Ψi.
G = (2|ΨihΨ| − I)(I − 2|aiha|).
|ai
W V |Ψi
Consider the actions of W and V on the two states |Ψi and |ai.
W |Ψi = |Ψi
V |Ψi = |Ψi −
√2 |ai
N
W |ai =
√2 |Ψi
N
− |ai.
V |ai = −|ai
Thus, as we start the algorithm in state |Ψi, the result of repeated
applications of V and W will always give a real linear combination
of |ai and |Ψi.
2θ
θ
|Ψi
V |Ψi
V is a reflection
about the line perpendicular to |ai.
W is a reflection
about |Ψi.
The composition of
two reflections of the
plane is always a rotation.
13
The Rotation
Number of Iterations
√
π
After t ∼ π/2
∼
2θ
4 N iterations of the Grover iterate G = W V ,
the state of the system
It is clear from the picture that W V (the Grover iterate) is a
rotation through an angle 2θ in the direction from |Ψi to |ai, where
the angle between |Ψi and |ai is π2 − θ.
Gt |Ψi
is within an angle θ of |ai.
|Ψi and |ai are nearly orthogonal, so θ is small (if N is large).
sin θ = cos(
14
A measurement at this stage yields the state |ai with probability
1
π
1
− θ) = ha|Ψi = √ = n/2 .
2
2
N
|hGt Ψ|ai|2 ≥ (cos θ)2 = 1 − (sin θ)2 =
N −1
.
N
So,
1
1
θ ∼ √ = n/2
2
N
for large enough values of N .
Note: Further iterations beyond t will reduce the probability of
finding |ai.
15
Multiple Solutions
Grover’s algorithm works even if the solution |ai is not unique.
Suppose there is a set of solutions S ⊆ {0, . . . , N − 1} and let
M = |S| be the number of solutions.
The Grover iterate is then a rotation in the space spanned by the
two vectors
N −1
1 X
√
|Ψi =
|ii
N i=0
1 X
|Si = √
|ji
M j∈S
As the angle between these is smaller, the number of iterations
drops, but so does the probability of success.
16
Lower Bound
For classical algorithms, searching an unstructured space of
solutions (such as given by a black box for f ), it is easy to show a
Ω(N ) lower bound on the number of calls to the black box required
to identify the unique solution.
Grover’s algorithm demonstrates that a quantum algorithm can
beat any classical algorithm for the problem.
√
It is possible to show a Ω( N ) lower bound for the number of calls
to Uf by any quantum algorithm that identifies a unique solution.
Grover’s algorithm does not allow quantum computers to solve
NP-complete problems in polynomial time.
1
2
Quantum Factoring
Quantum Computing
Lecture 7
A polynomial time quantum algorithm for factoring numbers was
published by Peter Shor in 1994.
Anuj Dawar
polynomial time here means that the number of gates is
bounded by a polynomial in the number of bits n of the
number being factored.
Quantum Factoring
The best known classical algorithms are exponential (in n1/3 ).
Fast factoring would undermine public-key cryptographic systems
such as RSA.
3
Period Finding
Suppose we are given a function f : N → {0, . . . , N − 1} which we
know is periodic, i.e.
4
Order Finding
Suppose we are given an integer N and an a with a < N and
gcd(a, N ) = 1.
f (x + r) = f (x) for some fixed r and all x.
Can we find the least value of r?
If we can find the period of a function efficiently, we can factor
integers quickly.
Consider the function fa : N → {0, . . . , N − 1} given by
fa (x) ≡ ax
(mod N )
Then, fa is periodic, and if we can find the period r, we can factor
N.
5
6
Factoring
Factoring–contd.
Suppose (for simplicity) N = pq, where p and q are prime. And, for
some a < N , we know the period r of the function fa .
r+1
Then, a
So, (x − 1)(x + 1) = kpq for some k.
Now, finding gcd(N, x − 1) and gcd(N, x + 1) will find p and q.
r
≡ a (mod N ), so a ≡ 1 (mod N ).
If r is even and a
r/2
If we randomly choose a < N
2
r
+ 1 6≡ 0 (mod N ), then take x = a .
x2 − 1 ≡
(x − 1)(x + 1) ≡
(and check that gcd(a, N ) = 1—if not, we’ve already found
a factor of N )
0 (mod N )
then, there is a probability >
0 (mod N )
1
2
that
• the period of fa is even; and
But,
• ar/2 + 1 6≡ 0 (mod N ).
x − 1 6≡ 0 (mod N ) (by minimality of r)
x + 1 6≡ 0 (mod N ) (by assumption)
7
8
Using a Fourier Transform
A fast period-finding algorithm allows us to factor numbers quickly.
The idea is to use a Fourier Transform to find the period of a
function f .
Note, classically, we can use the fast Fourier transform algorithm
for this purpose, but it can be shown that this would require time
N log N , which is exponential in the number of bits of N .
Discrete Fourier Transform
The discrete Fourier transform of a sequence of complex numbers
x0 , . . . , xM −1
is another sequence of numbers
y0 , . . . , yM −1
where
M −1
1 X
yk = √
xj e2πijk/M
M j=0
or
M −1
1 X
yk = √
xj ω jk .
M j=0
where ω = e2πi/M .
9
10
DFT is Unitary
Inverse DFT
The discrete Fourier transform is a unitary operation on CM .
The inverse of the discrete Fourier Transform is given by:


1
1
1
···
1


 1 ω −1
ω −2
···
ω 




−2
−4
2

ω
···
ω
1 
 1 ω

−1
D =√ 

−3
−6
3


1
ω
ω
·
·
·
ω
M

 .

..
..
..
..
 ..

.
.
.
.


Writing ω for e2πi/M ,
ω, ω 2 , . . . , ω M −1 , ω M = 1
are the M th roots of 1.





1 

D= √ 
M




1
1
1
1
ω
ω2
1
ω2
ω4
1
..
.
ω3
..
.
ω6
..
.
1
ω M −1
ω 2M −2
···
1


· · · ω −1 


−2 
··· ω


· · · ω −3 

.. 
..
.
. 

···
ω
1 ω 1−M
ω 2−2M
· · · ω M −1
Exercise: Verify that D is unitary. Verify that D −1 as given above
is the inverse of D.
11
12
Quantum Fourier Transform
Computing the discrete Fourier transform classically takes time
polynomial in M .
Fourier Transform on Binary Strings
Suppose M = 2n , and let |xi be a computational basis state in CM
with binary representation x1 · · · xn .
Let
Shor showed that D can be implemented using a number of one and
two-qubit gates that is only polynomial in the number of qubits
O((log M )2 ).
ηj = e2πi(0·xj xj+1 ···xn ) .
Then
Note: This does not give a fast way to compute the DFT on a
quantum computer.
There is no way to extract all the complex components from the
transformed state.
D|xi = (|0i + ηn |1i)(|0i + ηn−1 |1i) · · · (|0i + η1 |1i).
Exercise: Verify.
13
14
Quantum Fourier Transform Circuit
Conditional Phase Shifts
Here
We can use this form to implement the quantum Fourier transform
using Hadamard gates and conditional phase-shift gates.

P =
H
H
P
H
H
P
Q
1
0

0
i


Q=
1
0

0
eiπ/4


R=
1
0
0 eiπ/8


Two-qubit conditional phase shift gates are actually symmetric
between the two bits, despite the asymmetry in the drawn circuit.
P
Q
It seems that for large n, an n-bit quantum Fourier transform
circuit would require conditional phase shifts of arbitrary precision.
R
It can be shown that this can be avoided with some (but not
significant) loss in the probability of success for the factoring
algorithm.
In the input, the least significant bit is at the top, in the output, it
is at the bottom.
15
16
Preparing the State
We are given an implementation of the function f as a unitary
operator Uf
|xi
|0i
Uf
First Measurement
We measure the second n qubits of the state Uf |Ψi|0n i and get a
value f0 . The state after measurement is:
Where, now, each of the two input wires represents n distinct
qubits
|xi
|f (x)i
m−1
1 X
√
|x0 + kri |f0 i.
m
k=0
where:
Writing |Ψi for the state
H ⊗n |0n i =
1
2n/2
n
2X
−1
x=0
x0 is the least value such that f (x0 ) = f0
|xi.
We have,
n
Uf |Ψi|0 i =
1
2n/2
n
2X
−1
x=0
|xi|f (x)i.
r is the period of the function f
n
m = ⌊ 2r ⌋.
17
Applying the QFT
Second Measurement
We apply the n-qubit quantum Fourier transform to the first n bits
of the transformed state.
√1
m
D
=
1
m−1
X
|x0 + kri
k=0
n
2X
−1
2n/2
y=0
=
n
2X
−1
y=0
where ω = e
2πi/2n
ω
x0 y
18
The probability of observing a given state |yi is:
m−1
2
1 X kry ω .
2n m k=0
m−1
1 X (x0 +kr)y
√
ω
|yi
m
This probability function has peaks when ry/2n is close to an
integer.
k=0
m−1
X
1
kry
√
ω
|yi.
2n/2 m k=0
Indeed, if ry/2n is an integer, then the probability of measuring y
is 1.
.
Given an integer multiple of 2n /r, it is not difficult to find r.
19
Exponentiation
20
Some Points to Note
To complete the factoring algorithm, we need to check that we can
also implement the unitary transform Uf for the particular function
The two measurement steps can be combined at the end, with the
Fourier transform applied before the measurement of f (x).
fa (x) = ax mod N.
The probability of successfully finding the period in any run of the
algorithm is only about 0.4.
with a number of quantum gates that is polynomial in log N .
This is achieved through repeated squaring.
However, this means a small number of repetitions will suffice to
find the period with high probability.
Putting a lower bound on the conditional phase shift we are allowed
to perform affects the probability of success, but not the rest of the
algorithm.
1
2
Models of Computation
Quantum Computing
Lecture 8
Shor’s algorithm solves, in polynomial time, a problem for which no
classical, deterministic polynomial time algorithm is known.
Anuj Dawar
What class of problems are solvable by quantum machines in
polynomial time?
Quantum Automata and Complexity
More generally, how does quantum parallelism compare with other
forms of parallelism and nondeterminism.
How does the quantum model of computation affect our
understanding of complexity classes?
3
Finite State Systems
a
a
Its operation can be described by a
pair of matrices.
b

Ma = 
1 0
0 1
DFAs and Matrices
This automaton accepts the set of
strings that contain at least one b.
b


4

Mb = 
0
1
0
1


Mb Mb Ma describes the operation on states performed by reading
the string abb.
Each DFA is specified by a collection of n × n matrices, where n is
the number of states in the DFA, and there is one matrix for each
letter.
Each column of each matrix is a unit vector with 0, 1
entries.
More generally, we can form a matrix Mw for each word w.
Multiplication of matrices corresponds to concatenation of
words.
Mw |ii = |ji if there is a path labelled w from state i to state j.
5
Nondeterministic Automata
a
b
b
Ma = 

Mbb = 
The columns of the corresponding
matrices are no longer unit vectors.
b

NFAs and Matrices
This automaton accepts the same
set of strings as the deterministic
one.
a
1 0
0 1


Mb = 

1
1
6
0
1
1 0
2 1


Mw (i, j) gives the number of paths labeled w from state i to state j.

Mw |ii =

X
Mw (i, j)|ji
j
7
Probabilistic Automata
Language Accepted
We obtain probabilistic automata if we allow fractional values in
Mσ .
with the proviso that each column adds up to 1.
E.g.

Ma = 

M a Mb = 
0.5 0.0

0.5 1.0

0.4

0.6
0.1
0.9


Mb = 
0.8 0.2
0.2 0.8
8


gives, in position (i, j) the probability that string ba takes you
from state i to state j.
A probabilistic automaton A accepts a language L with certainty if

 1 if w ∈ L
P (A accepts w) =
 0 if w 6∈ L
A accepts a language L with bounded probability if there is an
ǫ < 1/2 such that:

 > 1 − ǫ if w ∈ L
P (A accepts w) =
 <ǫ
if w 6∈ L
The class of languages accepted by probabilistic automata (under
either definition) is the regular languages.
9
10
Quantum Automata
Acceptance Probabilities
Quantum finite automata are obtained by letting the matrices Mσ
have complex entries.
If q is the starting state of the automaton,
Mw |qi
We also require each of the matrices to be unitary.
E.g.

Mσ = 
−1 0
0
i


is the state after reading w. If
Mσ is unitary since the sum of
the squares of the norms in each
column adds up to 1 and the dot
product of any two columns is 0.
αj = hj|Mw |qi
then αj is the probability amplitude that the automaton reaches
state j.
|αj |2 is the probability that a measurement will result in
state qj .
P
2
j∈F |αj | is the probability that the automaton accepts
the string w.
NB: If all matrices only have 0 or 1 entries and the matrices are
unitary (i.e., the matrices are permutation matrices), then the
automaton is deterministic and reversible.
11
12
Language Accepted
We can define language acceptance exactly or by bounded
probability.
Interference
Consider the automaton in a one letter alphabet defined as:
√1
2
√1
2
− √12
Because of the reversibility requirement, quantum automata are
quite a weak model.
There are regular languages that cannot be accepted by a QFA.
However, QFAs may be much more succinct than their classical
counterparts.
q1
q2
√1
2

Maa = 
0
1
−1
0



Ma = 
√1
2
−1
√
2
√1
2
√1
2


While there are two distinct paths labelled aa from q1 back to itself, and each
has non-zero probability, the net probability of ending up in q1 is 0.
The automaton accepts a string of odd length with probability 0.5
and a string of even length with probability 1 if its length is not a
multiple of 4 and probability 0 otherwise.
13
Turing Machines
14
Configurations and Computations
A Turing machine, in addition to the finite set of states in the
automaton has an infinite read-write tape.
If c0 is the configuration in the starting state, with w on the tape
and the tape head at the left end of the string, w is accepted if the
computation
c0 → c 1 → · · · → c f
A machine is determined by an alphabet Σ, a finite set of states Q
and a transition function δ which gives, for each state and symbol:
a next state, a replacement symbol and a direction in which to
move the tape head.
eventually reaches an accepting state.
If the length of the computation is bounded by a polynomial in the
length of w, the language accepted by the machine is in P.
A machine has infinitely many possible configurations (reserving
the word “state” for a member of Q).
The action of the Turing machine can equivalently be described as
a linear operator M on an infinite-dimensional space.
Each configuration c is determined by a state, the contents of the
tape (a finite string) and the position of the head.
The set of configurations form a basis for the space.
15
Nondeterministic Turing Machines
In a nondeterministic machine, δ determines, for each state and
symbol, a set of next moves.
This gives rise to a tree of configurations:
c4
c1
c5
A configuration may occur in several
places in the tree.
c6
c2
c0
c7
The initial string w is accepted by the mac8
chine if there is some path through the
c9
tree leading to an accepting state.
c3
c10
If the height of the tree is bounded by a polynomial in the length of
w, then the language is in NP
16
Probabilistic Machines
With a probabilistic machine, δ defines, for each current state and
symbol, a probability distribution over the possible next moves.
The action of the machine can be defined as an infinite matrix,
where the rows and columns are configurations, and each column
adds up to 1.
However, how much information can be encoded in a single entry?
We require the entries α to be feasibly computable. That is, there is
a feasibly computable f such that:
|f (n) − α| < 2−n
17
18
BPP
Quantum Turing Machines
BPP is the collection of languages L for which there is a
probabilistic machine M , running in polynomial time with:

 > 2 if w ∈ L
3
P (M accepts w) =
 < 1 if w 6∈ L
With a Quantum Turing machine, δ associates with each state and
symbol, and each possible next move, a complex probability
amplitude (which we require to be a feasible complex number).
c4
3
c1
The class of languages is unchanged if we replace 23 and 13 by 1 − ǫ
and ǫ, for any ǫ < 12 , or indeed the set of all feasibly computable
probabilities with {0, 12 , 1}.
α0
c
c0 α1 2
α2
The only inclusion relations we know are P⊆NP and P⊆BPP.
c5
c6
c7
c3
Note that the probability of c7 occurring
at time 2 may be less than the sum of the
probabilities along the two paths.
c8
c9
Primality testing, long known to be in NP and in BPP was shown
in 2002 to be in P.
The machine can be seen as progressing
through a series of stages, each of which
is a superposition of configurations.
We also require that the linear transformation defined by the machine is unitary.
19
20
BQP
BQP is the collection of languages L recognised by a quantum
Turing machine, running in polynomial time, under the bounded
probability rule.
The class BQP is not changed if we restrict the set of possible
amplitudes to {0, ± 35 , ± 54 , 1}.
Complexity Classes
factorisation
NP − C
PSPACE
NP
BPP
P
BQP
BPP ⊆ BQP
Inclusion relations among the complexity classes as we know them.
Shor’s algorithm shows that the factorisation problem is in BQP.
It is not known to be in BPP.